Jump to
S1C2
Energy calculated at LSDA/6-311G**
| | hartrees |
| Energy at 0K | -90.094030 |
| Energy at 298.15K | -90.093496 |
| HF Energy | -90.094030 |
| Nuclear repulsion energy | 17.656192 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at LSDA/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.022 |
-0.353 |
0.000 |
| Be2 |
0.022 |
1.023 |
0.000 |
| H3 |
-0.259 |
-1.267 |
0.000 |
Atom - Atom Distances (Å)
| |
O1 |
Be2 |
H3 |
| O1 | | 1.3754 | 0.9564 |
Be2 | 1.3754 | | 2.3067 | H3 | 0.9564 | 2.3067 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Be2 |
O1 |
H3 |
162.922 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.470 |
|
|
|
| 2 |
Be |
0.190 |
|
|
|
| 3 |
H |
0.279 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.545 |
-1.517 |
0.000 |
1.612 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.068 |
0.837 |
0.000 |
| y |
0.837 |
-11.208 |
0.000 |
| z |
0.000 |
0.000 |
-12.268 |
|
| Traceless |
| | x | y | z |
| x |
-0.330 |
0.837 |
0.000 |
| y |
0.837 |
0.960 |
0.000 |
| z |
0.000 |
0.000 |
-0.631 |
|
| Polar |
| 3z2-r2 | -1.261 |
| x2-y2 | -0.860 |
| xy | 0.837 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.567 |
0.092 |
0.000 |
| y |
0.092 |
4.351 |
0.000 |
| z |
0.000 |
0.000 |
4.515 |
<r2> (average value of r
2) Å
2
| <r2> |
14.257 |
| (<r2>)1/2 |
3.776 |
Jump to
S1C1
Energy calculated at LSDA/6-311G**
| | hartrees |
| Energy at 0K | -90.094018 |
| Energy at 298.15K | |
| HF Energy | -90.094018 |
| Nuclear repulsion energy | 17.687751 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at LSDA/6-311G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| O1 |
0.000 |
0.000 |
0.348 |
| Be2 |
0.000 |
0.000 |
-1.023 |
| H3 |
0.000 |
0.000 |
1.304 |
Atom - Atom Distances (Å)
| |
O1 |
Be2 |
H3 |
| O1 | | 1.3714 | 0.9555 |
Be2 | 1.3714 | | 2.3269 | H3 | 0.9555 | 2.3269 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Be2 |
O1 |
H3 |
180.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.470 |
|
|
|
| 2 |
Be |
0.194 |
|
|
|
| 3 |
H |
0.276 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
1.642 |
1.642 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.262 |
0.000 |
0.000 |
| y |
0.000 |
-12.262 |
0.000 |
| z |
0.000 |
0.000 |
-10.970 |
|
| Traceless |
| | x | y | z |
| x |
-0.646 |
0.000 |
0.000 |
| y |
0.000 |
-0.646 |
0.000 |
| z |
0.000 |
0.000 |
1.292 |
|
| Polar |
| 3z2-r2 | 2.584 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.517 |
0.000 |
0.000 |
| y |
0.000 |
4.517 |
0.000 |
| z |
0.000 |
0.000 |
4.374 |
<r2> (average value of r
2) Å
2
| <r2> |
14.247 |
| (<r2>)1/2 |
3.775 |